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This is similar to a DOE, which is a sampled device Hence, the images repeat at certain intervals This limits the number of wavelengths that can be imaged without interference from other wavelengths A method called irregularly sampled zero-crossings (MISZCs) is discussed to avoid this problem The MISZC has its origin in one-image-only holography discussed in 15 Scalar diffraction theory becomes less accurate when the sizes of the diffracting apertures are smaller than the wavelength of the incident wave Then, the Maxwell equations need to be solved by numerical methods Some emerging approaches for this purpose are based on the method of nite differences, the Fourier modal analysis, and the method of nite elements The rst two approaches are discussed in 20 First, the paraxial BPM method discussed in Section 124 is reformulated in terms of nite differences using the Crank-Nicholson method.

If trend following is such a successful methodology, how can indicators based on the exact opposite philosophy generate consistent profits The simple answer is that mean reversion indicators, such as RSI and other oscillators, work because they capitalize on the market s tendency to overextend itself. Whether the trend has matured and is approaching climactic reversal or is still in its infancy and simply correcting a temporarily overbought or oversold condition, the market has an uncanny knack for separating the less experienced from their money by exploiting their greed, lack of patience, and complacency. Imagine speculators who saw the bull move early but allowed fear of losses to prevent them from buying the market. As the trend matures, their anxiety and regret magnify in lockstep with forfeited profits until they finally capitulate and buy at any price so that they can participate in this once-in-a-lifetime trend. Since the thought process that accompanied their ultimate trading decision was purely emotional and devoid of price risk management considerations, when the inevitable pullback or change in trend occurs, greed and hysteria quickly shift to panic and capitulation. Although mean reversion indicators such as oscillators attempt to somehow quantify these unsustainable levels of market emotionalism, they

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Next, the wide-angle BPM using the Pade approximation is discussed The nal sections highlight the nite difference time domain and the Fourier modal method Many colleagues, secretaries, friends, and students across the globe have been helpful toward the preparation of this manuscript I am especially grateful to them for keeping me motivated under all circumstances for a lifetime I am also very fortunate to have worked with John Wiley & Sons, on this project They have been amazingly patient with me Without such patience, I would not have been able to nish the project Special thanks to George Telecki, the editor, for his patience and support throughout the project..

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The aperture locations (xi , yi ) can be chosen such that the resulting yi will be a constant. An object point is then obtained since all wave fronts generated by the hologram apertures will add up in phase at the speci ed object point location. Thus, the amplitude of the eld will be proportional to dx dy N, and its phase will be 0 for a plane incoming wave incident on the hologram at right angle. If there are groups of such apertures that satisfy Eq. (15.8-6) at different points in space, a sampled wavefront is essentially created with a certain amplitude and phase at each object point. We note that the modulation of Eq. (15.8-6) is very simple. We vary dx and/or dy and/or N for amplitude and y for phase. The fact that N is normally a large number means that it can be varied almost continuously so that amplitude modulation can be achieved very accurately. If amplitude modulation accuracy does not need to be very high, the method is valid in the near eld as well because roi is exactly computed for each object point. If the apertures are circular, the sinc functions are replaced by a rst-order Bessel function, but Eq. (15.8-6) essentially remains the same. In practice, each point-aperture on the hologram plane is rst chosen randomly and then moved slightly in the x- and/or y-direction so that its center coordinates satisfy Eq. (15.8-7) with constant y. Overlapping of the apertures is considered negligible so that there is no need for using memory. 15.8.1 Experiments

In some ways, ACM and LTCM seem entirely different. ACM seems to have failed because of basic incompetence and a lack of analytical tools. LTCM seems to have failed because more than competent professionals placed more than warranted reliance on sophisticated analytical tools.

He who has eyes to see and ears to hear may convince himself that no mortal can keep a secret. If his lips are silent, he chatters with his ngertips; betrayal oozes out of him at every pore (Freud, 1959, p. 94).

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